SERS chemical enhancement by copper - Nanostructures: Theoretical study of Thiram pesticide adsorbed on Cu₂₀ cluster
Cite this paper: Vietnam J. Chem., 2021, 59(2), 159-166
DOI: 10.1002/vjch.202000137
Article
SERS chemical enhancement by copper - nanostructures: Theoretical
study of Thiram pesticide adsorbed on Cu20 cluster
Truong Dinh Hieu1,2, Ngo Thi Chinh1,2, Nguyen Thi Ai Nhung3, Duong Tuan Quang4,
Dao Duy Quang1,5*
1Institute of Research and Development, Duy Tan University, Da Nang, 50000, Viet Nam
2Faculty of Natural Sciences, Duy Tan University, Da Nang, 50000, Viet Nam
3Department of Chemistry, University of Sciences, Hue University, Hue City, Thua Thien Hue 49000, Viet Nam
4University of Education, Hue University, Hue City, Thua Thien Hue 49000, Viet Nam
5Department of Environmental and Chemical Engineering, Duy Tan University, Da Nang, 50000, Viet Nam
Submitted August 7, 2020; Accepted November 9, 2020
Abstract
Surface-enhanced Raman spectroscopy (SERS), a surface-sensitive technique, allows the practicability of detecting
chemical compounds in ultra-low concentration. In this work, a chemical enhancement mechanism of SER process of
Thiram pesticide adsorbed on copper nanomaterial surface was proposed based on density functional theory (DFT)
approaches. Structural and electronic properties of Thiram and Thiram-Cu20 complexes were optimized using PBE
method with LanL2DZ basis set for copper atoms and cc-pVDZ basis set for the non-metal atoms. In the most stable
adsorption configuration, Thiram interacted with Cu20 cluster via two S(sp2) atoms. The main peaks on normal Raman
spectrum of Thiram were characterized at 371, 576, 1414 and 1456 cm-1 responsible for the stretching vibrations of
C–S, C=S, S–C–S and C–N groups, respectively. Otherwise, the main peaks of Thiram-Cu20 SERS spectrum were
found at 534, 874, 982, 1398 and 1526 cm-1 corresponding to the stretching vibrations of S–S, C-S, S–C–S, C–N and
CH3–N bonds, respectively. The SERS chemical enhancement of Thiram by Cu20 cluster was about 2 and 6 times
stronger than those obtained from Ag20 and Au20 cluster, respectively. The chemical enhancement mechanism was also
explained by analyzing HOMO and LUMO energies gap and density of states.
Keywords. Thiram, copper cluster, Raman, SERS, DFT.
1. INTRODUCTION
This compound is also used to protect fruit trees and
ornamental fruits from damage of rabbit, rodent and
Pesticides are chemical compounds used in modern deer.[7]
agriculture to kill insects, fungus, bacteria, weed and
For many decades, surface-enhanced Raman
rodents. They are respectively named as insecticides, spectroscopy (SERS) has intensively been
fungicides, bactericides, herbicides and rodenticides. investigated
for
its
electromagnetic
field
By the structure, pesticides can be divided into enhancement near the nano-scale metallic surfaces
organochlorines, organophosphates, carbamates and of coinage metals (i.e. gold, silver and copper).
triazines.[1,2] An increasing utilization of pesticides Despite of intensive research attempts SERS
in agriculture results in several severe problems on chemical enhancement mechanism is still unclear
environment and human health.
mainly due to the relatively complicated enhancing
Thiram (tetramethyl-thiuram disulfide or factors and inconsistent experimental results. The
bis(dimethyl-thiocarbamoyl) disulfide) (C6H12N2S4) advantages of SERS are that it magnifies Raman
is a carbamate-categorized pesticide. Its molecular signals corresponding to the adsorbed compounds
structure has two dimethyl-dithio-carbamate groups from 106 to 1010 times. Therefore, SERS technique
– (CH3)2N–CS2 linked together by a disulfide bridge has increasingly been utilized to improve detection
(S–S). Thiram has been used in many countries as of chemicals at trace concentrations. Attracted by its
fungicide to protect fruits, vegetables, ornamental great advantages, many researches have employed
and turf crops from a variety of fungal diseases.[3-6] SERS to analyze different chemical pesticides,
159 Wiley Online Library © 2021 Vietnam Academy of Science and Technology, Hanoi & Wiley-VCH GmbH
Vietnam Journal of Chemistry
Dao Duy Quang et al.
including Thiram, accumulated either in the predicted and compared with the spectra obtained by
environment or in agricultural products. the corresponding investigations on Ag20 and Au20
Kang et al. analyzed the SERS spectrum of clusters in order to demonstrate the effectiveness of
Thiram adsorbed on silver surface.[8] Their results copper substrate for SERS technique. Finally, a
revealed that the peaks of Thiram located in the chemical enhancement mechanism is proposed
region below 1000 cm-1 (related to C–S, C–S–S providing more insight for SERS phenomenon. To
assignments) are decreased or even disappeared in the best of our knowledge, there have been an
the SERS spectrum; whereas, others characterized insignificant number of experimental and
for C–N and CH3NC are enhanced, especially C–N computational studies in the literature on SERS of
stretching mode at 1372 cm-1. These phenomena chemical compounds adsorbed onto the surface of
were also confirmed by Verma et al. using silver copper nanoparticles.
nanodendrites.[9]
The prediction of Raman and SERS spectra has 2. COMPUTATIONAL METHOD
commonly been investigated using density
functional theory (DFT). Metallic cluster models are All the DFT calculations were carried out using
often used to reproduce nanoparticle surface. The Gaussian 16, revision A.03.[12] The chosen DFT
complexes produced from interaction between an method was PBE[13] combined with the LanL2DZ
analyzed ligand and a metallic cluster can be utilized basis set for metallic atom (i.e. Cu, Au, Ag) and the
to predict their SERS spectra. Rajalakshmi et al. cc-pVDZ basis set for the non-metallic atoms.
determined geometrical and electronic structures of Different configurations of interactions between
2-propylpiridine-4-carbothioamide as well as studied Thiram and Cu clusters were analyzed. The most
infrared, Raman spectra.[10] In their work, various stable Thiram-Cu20 complex was used to project the
DFT functionals including PBEPBE, SVWN, corresponding SERS spectrum. It was then
HCTH, B3LYP, mPW1PW91, B3PW91 combined compared with the spectra obtained from Thiram-
with aug-cc-pVDZ basis set were chosen as Au20 and Thiram-Ag20 complexes in an attempt to
computational strategies for spectra prediction. The explain the influence of cluster nature on SERS
research indicated that the B3LYP/aug-cc-pVDZ enhancement. The scaling factor for harmonic
model results in the lowest deviations in the frequencies of PBE/cc-pVDZ method was 1.0353.[14]
prediction of structure and vibrational spectra. Gaussum[15] was used to investigate density of states.
Recently, An et al. investigated surface-enhanced
Raman scattering of melamine (C3H6N6) on silver 3. RESULTS AND DISCUSSION
substrate using experimental and DFT studies with
the B3LYP/6-31G(d) method.[11] Silver cluster
3.1. Structure of Thiram
models including Ag4, Ag8, Ag10 and Ag20 were used
to reproduce silver substrate. It was found that the Figure 2 shows optimized structure, the highest
small size clusters like Ag4 can be an effective occupied molecular orbital (HOMO), the lowest
predictor for Raman and SERS spectra of melamine. unoccupied molecular orbital (LUMO) distributions
This research also showed that the enhancement of and electrostatic potential (ESP) map of Thiram in
typical peaks localized at 676 and 983 cm-1 were vacuum. The experimental structural parameters of
correctly predicted and consistent with the Thiram are also included.
corresponding experimental results.
The structural parameters obtained from the
PBE/cc-pVDZ level of theory are in good agreement
with the experimental values. The difference
between the respective bond lengths varies from
0.020 to 0.042 Å, within the deviation of 1.4-2.8 %.
The calculated C11–S1–S2–C12 dihedral angle is
86.6o which is in accordance with the measurement
gained from experiments (i.e. 88.3o). In the C2NCS2
group, all the atoms are nearly coplanar given the
data S3–C11–N5–C7 = 4.7o, S1–C11–N5–C8 =
3.5o, S1–S3–C7–C8 = 4.2o. These imply a sp2 -
hybridized structure of N and C atoms. In fact, C7–
N5–C8 and C7–N5–C11 angles are equal to 118.6o
and 118.0o, respectively, which are far from the
characteristic angle of an sp3 hybridization (109.5o);
Figure 1: Molecular structure of Thiram
This study investigates Raman and SERS spectra
of Thiram pesticide (figure 1) adsorbed on copper
substrate using Cu20 cluster model. The Raman
spectrum of Thiram is projected and compared with
the experimental data from the literature. SERS
spectrum of Thiram adsorbed on Cu20 cluster is
Vietnam Journal of Chemistry
SERS chemical enhancement by copper - nanostructures:…
also S3–C11–N5 (124.9o) and S1–C11–S3 (124.0o) and the S(sp2) atoms of Thiram are predicted
angles are also close to 120o, the typical angle of an exhibiting high tendency to donate electrons.
sp2 hybridization. The bond angles at each S atom of Otherwise, LUMOs are mainly distributed around S,
S–S bridge (i.e. C12–S2–S1 and C11–S1–S2) are N and C(sp3) atoms. Thus, if a Thiram molecule is
102.5o. These values are smaller than sp3 angle allowed to interact with a metal cluster, these
(109.47o). The reason of this is the influence of two regions are expected to accept electrons and form an
free electron pairs in each S atom. These electron interactive bond. The results are also highly
pairs occupy large space and make the C–S–S bond consistent with those gained from ESP map.
angle smaller. But this difference is not too big.
If Thiram is adsorbed onto the surface of a
copper crystal, electron transfer may occur. In detail,
the regions in the adsorbent molecule localized by
high negative potential or large HOMOs may
interact with the copper cluster via donation of
electrons to the clustering atoms. Reversely, the
regions owing high positive charge or large LUMOs
are predicted to accept electrons transferred from
copper cluster. The stronger electronic exchange
formed, the more stable the complexes. In particular,
Thiram may interact with copper cluster via the
position of atoms S, especially at the S(sp2) atoms.
Therefore, S1 and S2 are in sp3 hybridization.
3.2. Structure of Thiram-Cu20 complexes
Figure 3 shows structures and relative energies of
seven complexes representing for all possible
interactions between a Thiram molecule and Cu20
cluster. Relative energy of each complex is
calculated by the difference of the according
enthalpy value with the lowest one.
Figure 2: (A) Optimized structure, (B) ESP map,
(C) HOMO and (D) LUMO of Thiram. Bond
lengths are in Å, angles are in degree. Values in
parentheses highlighted in red color are
experimental values of Kang et al.[8]
Thiram molecule attends to interact with at a
edge of pyramidal Cu20 cluster via two or three
sulfur atoms. The interacting modes A and B are
obtained by the complexation between two S(sp2)
atoms (i.e. S3 and S4) with two copper atoms. In
detail, the complex A comprises the interactions
occurring at top of the cluster, and the interaction in
complex B is observed at the center of one edge on
the pyramidal cluster. Mode A is the most stable
complex with the lowest relative energy (∆E = 0.0
kcal/mol). This is followed by mode B with the
value of ∆E 4.2 kcal/mol higher. Modes C (∆E = 7.4
kcal/mol) and D (∆E = 12.9 kcal/mol) correspond to
the interactions at S2 and S3 atoms with two other
respective copper atoms located at the top and at the
edge of the copper clusters, respectively. Finally, the
adsorption modes E, F and G are built through the
interactions between 3 sulfur atoms (one S(sp2) atom
and two S(sp3) atoms) with the copper cluster. The
relative energies of these modes are significantly
higher than the energy of mode A, varying within
9.6-12.6 kcal/mol. Thus, a Thiram-Cu20 complex is
predicted most stable if the S(sp2) atoms in the
Thiram molecule interact with cluster-copper atom
at the top of the cluster.
The ESP map given by figure 2B illustrates the
charge distribution of molecules in a three-
dimentional
simulation,
which
allows
a
determination on how the molecule interacts with
exotic agents. In principle, the regions colorized in
red represent the most negative atomic zones, prone
to be attacked by electrophilic species; whilst, blue
regions exhibit the most positive charges, conducive
to an interaction with nucleophile species. This
suggests that the S(sp2) atoms possess the highest
negative potential due to the +M effect of
neighboring N and S(sp3) atoms, while the most
positive potential is observable localizing at SS and
CH3 groups. The high significance of positive charge
at these groups can be explained by the –M effect of
the C=S bond and the electron deficiency on N
atom. Therefore, S(sp2) atoms are expected to donate
electrons to an external electrophilic agent; whereas,
S–S and CH3 groups can are more likely to accept
electrons from a nucleophilic counterpart.
HOMO and LUMO distributions in Thiram
structure are shown in Figures 2C and 2D. HOMOs
localize around the C–S–S–C group and two S(sp2)
atoms. Besides, N and C(sp3) atoms are surrounded
by smaller HOMOs. Therefore, the C–S–S–C group
Vietnam Journal of Chemistry
Dao Duy Quang et al.
In addition, the S(sp2) atoms are more favorable molecule and Cu20 cluster may perform quasi-
to approach the cluster than their sp3– hybridization covalent characteristics, conducive to the stability of
counterparts. The interactive distances between the bonding, especially formed by complex A.
S(sp2) atom (i.e. S3 and S4) and copper atoms vary
In the next section, the SERS spectrum of the
between 2.33-2.50 Å while the corresponding complex A in comparison with the normal Raman
figures for S(sp2) atoms (i.e. S1 and S2) are in the spectrum of Thiram are projected in order to propose
range 2.44-2.75 Å. These values the covalent bond a chemical enhancement mechanism of Thiram
distance of Cu-S (2.37 Å).[16] Therefore, in these adsorbed on the a Cu20 cluster.
complexes, the interactions between a Thiram
Figure 3: Optimized structures and relative energies (E, in kcal/mol) of seven Thiram-Cu20 complexes
A-G. Unit of distance is Å
differences with the normal Raman spectrum should
be noted. In figure 4B, the most marked peak is
3.3. Normal Raman and SERS spectra
Figure 4 compared Raman spectrum of Thiram found at 982 cm-1 and the other significant peaks are
(figure 4A) and SERS of the most stable Thiram- also detected at 534, 1398 and 1526 cm-1. They are
Cu20 (figure 4B), Thiram-Ag20 (figure 4C) and Au20- assigned to the stretching vibrations of S–S, S–C–S,
Thiram complexes (figure 4D). In addition, the C–N, CH3–N bonds; the scissoring bending
Raman and SERS vibrational assignments are listed vibrations of CH3NCH3, CH3NC groups and the
in table 1.
In normal Raman spectrum (figure 4A), the
wagging vibrations of CH3, CH3NCH3 groups.
The similar patterns are observed in SERS
highest peak emerges at 1456 cm-1 and five other spectra represented for Thiram-Ag20 (figure 4C) and
highly pronounced peaks are at 371, 576, 1012, 1414 Thiram-Au20 (figure 4D). Nevertheless, they
and 1430 cm-1. They are responsible for the experience a slight westward-shift and register a
stretching vibrations of C–S, C=S, S–C–S and C–N lower overall intensity.
bonds accompanied with the scissoring bending
By interacting with the metallic clusters, certain
vibrations of CH3 and CH3NC groups. Regarding the characteristic peaks of Thiram are enhanced. These
SERS spectra of Thiram-Cu20 (figure 4B), Thiram- especially include those at 553 cm-1 (which is nearly
Ag20 (figure 4C) and Thiram-Au20 (figure 4D), some negligible in normal Raman spectrum of Thiram),
Vietnam Journal of Chemistry
SERS chemical enhancement by copper - nanostructures:…
1012 cm-1, 1414 cm-1 and 1531 cm-1 (table 1). The 1.2 to 2.4 times higher than those of Thiram-Ag20
Raman intensities of these peaks see a respective and from 3.3 to 4.2 times higher than those of
rise of 122, 102, 50 and 175 times in the SERS Thiram-Au20.
spectrum of Thiram-Cu20 complex. Otherwise, the
indices for Raman enhancement vary from 21 to 104
times for Thiram-Ag20 complex and from 12 to 54
times for Thiram-Au20 complex. The enhancement is
mainly due to the stretching vibrations of CH3N, CN
groups and the wagging vibrations of CH3,
CH3NCH3 groups. However, some other peaks only
witness a marginal-to-non enhanced intensity, such
as those at 371, 576, 1430 and 1456 cm-1 (figure
4A). In particular, two peaks at 371 and 1430 cm-1
are both disappeared in the SERS spectra obtained
from all three metal complexes. These peaks relate
to the stretching vibration of C–S bond and the
scissoring bending vibrations of CH3, CH3NC
groups (table 1).
In addition, the Raman intensity of highest peak
in SERS spectrum of Thiram-Cu20 at 982 cm-1 is 2
times higher than that of Thiram-Ag20 and 6 times
higher than that of Thiram-Au20. The other
noticeable peaks of Thiram-Cu20 complex (i.e. 534,
1398 and 1526 cm-1) also have higher Raman
Figure 4: (A) Raman spectrum of Thiram and SERS
activities than the ones of other complexes. Overall,
Raman figures obtained for Thiram-Cu20 are from
spectra of the most stable complexes: (B) Thiram-
Cu20, (C) Thiram-Ag20 and (D) Thiram-Au20
Table 1: Vibrational assignments of normal Raman spectrum of Thiram and SERS spectra of Thiram
adsorbed on Cu20, Ag20 and Au20 clusters
Raman
SERS-Cu20
279 (80.2)
–
445 (76.6)
490 (171.3)
534 (439.9)
571 (109.9)
874 (238.8)
SERS-Ag20
236 (47.2)
–
SERS-Au20
210 (60.0)
–
401 (20.1)
–
538 (122.3)
557 (66.3)
870 (38.4)
983 (339.7)
1090 (8.3)
1155 (26.5)
1267 (12.9)
1399 (248)
–
Assignments
ρ(CH3), σ(NCS), σ(CSS)
υ(CS), σ(CH3NC)
301 (6.0)
371 (14.3)
451 (2.5)
–
553 (3.6)
576 (24.9)
873 (3.3)
396 (39.9)
525 (129.1)
540 (356.1)
559 (206.1)
871 (105.2)
991 (984.2)
1092 (12.4)
1159 (23.3)
1274 (58.8)
σ(CS), σ(NCS), σ(CH3NC),
ω(SCS), ω(CH3NCH3)
υ(SS), ω(SCS), ω(CH3NCH3)
σ(CH3NCH3), υs(SCS), υas(CSS)
υs(CH3NCH3), υs(CS)
υas(SCS), ω(CH3), υ(CH3N), σ(CH3NC)
ρ(CH3), ω(CH3)
ω(CH3), ρ(CH3), υas(SC=S)
υas(CH3NCH3), ω(CH3), υas(SCS)
υ(CN), ω(CH3)
1012 (18.9) 982 (1924.5)
1102 (4.3)
1178 (1.8)
1297 (1.9)
1126 (103.9)
1161 (84.0)
1272 (112.6)
1414 (20.7) 1398 (1041.7) 1398 (440.6)
1430 (14.4)
1456 (50.4) 1455(157.6)
1531 (3.6) 1526 (630.4)
–
–
σ(CH3)
σ(CH3)
υ(CN), ω(CH3), σ(CH3)
1457 (53.7)
1549 (375.8)
1458 (46.8)
1554 (193.3)
Values in parentheses are calculated Raman activities; (υ) = stretching (with υs = symmetric stretching and
υas = anti-symmetric stretching), σ = scissoring bending, ρ = rocking, ω = wagging, τ = twisting.
is based on the amplification of the light by the
excitation of localized surface plasmonic resonances
3.4. Chemical enhancement mechanism
It has been widely accepted that the SERS (LSPRs). The latter primarily refers to charge
phenomenon generally stems from electromagnetic transfer (CT) process, where the excitation
and chemical enhancement mechanisms. The former
wavelength resonates with the metalmolecule
Vietnam Journal of Chemistry
Dao Duy Quang et al.
charge transfer electronic states.[17] The chemical
enhancement mechanism of Thiram adsorbed on
Au20, Ag20 and Cu20 clusters is illustrated in figure 5
and table 2.
and LUMO one, i.e. HOMO-LUMO gap or E, is a
good indicator to evaluate kinetic stability and
chemical stability. Regarding table 2, the E values
of the bare clusters accord with the order: Au20
>
In particular, figure 5 summarizes total density
of states (DOS) spectrum of Thiram, Au20, Ag20 and
Cu20 bare clusters in comparison with the ones of
their complexes. The highest occupied molecular
orbital (HOMO) and the lowest unoccupied
molecular orbital (LUMO) distributions of the
studied structures are also displayed with their
corresponding energy values (EH and EL). The
extended values of HOMO-LUMO energy gap (E)
are also included. Furthermore, partial density of
states (PDOS) analyses provides contributing
proportion of Thiram and its coordinated metal
clusters in the complexes. LUMO and HOMO are
also indicated in order to analyze the CT tendency of
electron densities.
Ag20 > Cu20 with their corresponding figures 1.89,
1.67 and 1.46 eV, respectively. The narrowest
energy gap of Cu20 (1.46 eV) indicates its highest
reactivity towards Thiram in comparison with Au20
and Ag20 clusters. Expectedly, the HOMO-LUMO
energy gaps of the complexes are also in the similar
order: Thiram-Au20 (1.41 eV) > Thiram-Ag20 (1.28
eV) > Thiram-Cu20 (0.95 eV) which shows a reverse
order of the stability.
Thus, the narrower energy gaps of the Cu20 bare
clusters and of the Thiram-Cu20 complex are more
conducive transfer of electron densities from the
ligand to the cluster than those carried out by Ag20
and Au20 clusters. The easier electronic transfer also
explains for the most marked enhancement by SERS
for Thiram adsorbed on Cu20 (figure 4 and table 1).
Firstly, the difference between HOMO energy
Figure 5: Density of states (DOS) spectrum of Thiram, Au20, Ag20 and Cu20 bare clusters and their
complexes with Thiram (Thir-Au20, Thir-Ag20, Thir-Cu20). LUMO and HOMO distributions are presented on
the right and left hand sides of each graphic. The LUMO and HOMO energies are indicated besides the
vertical dotted lines with their HOMO-LUMO gap (E) in eV unit. The percentage values correspond to
contribution of Thiram and the metal clusters to LUMO and HOMO orbitals
Vietnam Journal of Chemistry
SERS chemical enhancement by copper - nanostructures:…
Secondly, information on the frontier orbitals of 4. CONCLUSIONS
the formed complexes clarifies the interaction
mechanism between the pesticide molecule and the Structural, electronic and spectroscopic properties of
clusters. And the most important interactions are Thiram and its complexes with Cu20, Ag20 and Au20
between HOMO and LUMO of Thiram and those of are computationally investigated using DFT method.
the clusters. Based on the energy gap, the donation or Normal Raman spectra of Thiram and SERS
back-donation of electrons can be revealed. Based on spectrum of its three complexes are projected. The
the calculated data in table 2, the energy differences results show that:
between LUMO of Thiram and HOMO of the clusters
are also ranged in declined order: Au20 > Ag20 > Cu20
with the respective values being 4.31, 3.27 and 3.16
eV. In contrast, the energy gaps between LUMO of
the Au20, Ag20 and Cu20 clusters and HOMO of
Thiram register are similar order but with
considerably smaller values i.e. 0.77, 1.59 and 1.49
eV, respectively. These imply that the HOMO-
LUMO energy gaps of the forward donation
(ThiramM20, with M represents the metal cluster)
are larger than the ones represented for backward
donations (M20Thiram). Hence, Thiram is adsorbed
on the metal cluster by donating its electron densities
to the cluster. This electron-transfer tendency from
organic molecules to metallic cluster is in agreement
with the previous studies.[18-20]
+ Thiram contains two co-planar C2NCS2 groups
and the interactive sites of Thiram are mainly found
at the its sulfur atoms (especially at S(sp2) atoms, i.e.
S3 and S4).
+ Thiram interacts with Cu20 cluster via two or
more sulfur atoms. The stability of Thiram-Cu20
complexes depends on the number of interaction
between Cu20 cluster and S(sp2) atom. The more
S(sp2) atom interact with the Cu20 cluster, the more
stable the complex is.
+ Normal Raman spectrum of Thiram shows
several main peaks including the stretching vibration
of C–S bond and scissoring bending vibration of
CH3 groups. Otherwise, the main peaks of SERS
spectrum of Thiram-Cu20, Thiram-Ag20 and Thiram-
Au20 complexes relate to N atom and the wagging
vibration of CH3 groups.
+ The SERS chemical enhancement for Thiram
derived by Cu20 cluster is 2 and 6 times higher than
those attained by Ag20 and Au20 clusters.
+ The most enhanced SERS signals of Thiram
adsorbed on Cu20 cluster are firstly related to its
lowest HOMO-LUMO energy gap by referencing to
the Au20 and Ag20 clusters. Moreover, during the
adsorption, the charge transfer prevails through the
forward donation direction from Thiram to the metal
clusters (ThiramM20). The energy gap between
LUMO of Thiram and HOMO of Cu20 is the lowest
compared with those of Au20 and Ag20 cluster. The
highest charge transfer from Thiram to cluster is also
obtained for the copper one. And this tends to the
highest SERS signals obtained when Thiram is
adsorbed on the Cu20 cluster.
Table 2: HOMO and LUMO energies and HOMO-
LUMO energy gap
HOMO
-4.72
-5.84
-4.80
-4.69
-4.94
-4.26
-3.94
LUMO
-1.53
-3.95
-3.13
-3.23
-3.53
-2.98
-2.99
E (eV)
3.19
Thir
Au20
1.89
Ag20
1.67
Cu20
1.46
Thir-Au20
Thir-Ag20
Thir-Cu20
1.41
1.28
0.95
This observation is further confirmed by
analyzing partial density of states (PDOS) (figure 5).
The contribution percentages of Thiram and the
clusters to LUMO and HOMO indicate that electron
densities are always transferred from Thiram to the
cluster during the transition from LUMO to HOMO
of the complexes. Regarding Thiram-Cu20, 75 of
LUMO electron density is localized on Thiram while
only 25 is found on the Cu20 cluster. However,
only 9 of HOMO electron density localizes on
Thiram, the corresponding figure for the cluster Cu20
is 91 %. This means that 64 electron densities are
transferred from Thiram to the Cu20 cluster.
Consistent phenomena are observed in regard to
Au20 and Ag20 clusters with the transfer of 16 and
73 electron densities, respectively.
The predicted results suggest a magnification-
enhanced
and
cost-effective
copper-based
nanomaterial as a potential alternative for expensive
inert metals, such as silver or gold, in SERS
applications. The most noticeable downside is its
sensitivity to ambient oxidization. The disadvantage
is less pronounced if the material is expected for
portable or one-use purposes.
Acknowledgments. This research is funded by
Vietnam National Foundation for Science and
Technology Development (NAFOSTED) under grant
number 103.03-2018.366.
Vietnam Journal of Chemistry
Dao Duy Quang et al.
in North America, CRC Press, Boca Raton: CRC
Press, 2017.
Conflict of interest. The authors declare no conflict
of interest.
8. J. S. Kang, S. Y. Hwang, C. J. Lee, M. S. Lee. SERS
of dithiocarbamate pesticides adsorbed on silver
surface; Thiram, Bull. Korean Chem. Soc., 2002, 23,
1604-1610.
9. A. K. Verma, R. K. Soni. Silver nanodendrites for
ultralow detection of thiram based on surface-
enhanced Raman spectroscopy, Nanotechnology,
2019, 30, 385502-385516.
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Corresponding author: Dao Duy Quang
Institute of Research and Development, Duy Tan University
3, Quang Trung, Da Nang, 50000, Viet Nam
E-mail: daoduyquang@duytan.edu.vn.
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